Final Magnetic Moment0.247 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingFM |
Formation Energy / Atom-1.162 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.052 eVThe energy of decomposition of this material into the set of most stable materials at this chemical composition, in eV/atom. Stability is tested against all potential chemical combinations that result in the material's composition. For example, a Co2O3 structure would be tested for decomposition against other Co2O3 structures, against Co and O2 mixtures, and against CoO and O2 mixtures. |
Density5.51 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToTi3Se4 |
Band Gap0.000 eVIn general, band gaps computed with common exchange-correlation functionals such as the LDA and GGA are severely underestimated. Typically the disagreement is reported to be ~50% in the literature. Some internal testing by the Materials Project supports these statements; typically, we find that band gaps are underestimated by ~40%. We additionally find that several known insulators are predicted to be metallic. |
Hermann MauguinC2/m [12] |
Hall-C 2y |
Point Group2/m |
Crystal Systemmonoclinic |
Topological ClassificationTI*
|
SubclassificationSEBR†
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Calculated powder diffraction pattern; note that peak spacings may be affected due to inaccuracies in calculated cell volume, which is typically overestimated on average by 3% (+/- 6%)
A full elastic tensor has not been calculated for this material. Registered users can view statistical-learning-based predictions of this material's bulk and shear moduli.
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Ti2VSe4 (mp-1025203) | 0.2108 | 0.016 | 3 |
Ti2CrTe4 (mp-1025345) | 0.2197 | 0.049 | 3 |
Cr(FeSe2)2 (mp-568349) | 0.2558 | 0.090 | 3 |
Ti2VTe4 (mp-1025219) | 0.2218 | 0.010 | 3 |
V2CrTe4 (mp-1025278) | 0.2656 | 0.042 | 3 |
Li4Ti2Mn3O10 (mp-766150) | 0.7273 | 0.042 | 4 |
Li3TiMn3O8 (mp-765898) | 0.6554 | 0.066 | 4 |
Li6Fe(O2F)2 (mp-777322) | 0.7433 | 0.093 | 4 |
Li4Fe2Cu3O10 (mp-849416) | 0.7182 | 0.097 | 4 |
Fe3Se4 (mp-569176) | 0.3646 | 0.079 | 2 |
V3S4 (mp-850014) | 0.3199 | 0.020 | 2 |
Fe3Se4 (mp-2780) | 0.3481 | 0.079 | 2 |
V3S4 (mp-1081) | 0.3627 | 0.020 | 2 |
V3Te4 (mp-1028) | 0.3767 | 0.016 | 2 |
Run TypeGGA |
Energy Cutoff520 eV |
# of K-pointsNone |
U Values-- |
PseudopotentialsVASP PAW: Ti_pv Se |
Final Energy/Atom-6.5430 eV |
Corrected Energy-45.8011 eV
-45.8011 eV = -45.8011 eV (uncorrected energy)
|
Displaying lattice parameters for primitive cell; note that calculated cell volumes are typically overestimated on average by 3% (+/- 6%). Note the primitive cell may appear less symmetric than the conventional cell representation (see "Structure Type" selector below the 3d structure)